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    Dr. Ottorino ORIDr. Ottorino ORIActinium Chemical ResearchActinium Chemical Research

    RomeRome

    [email protected]@gmail.com

    WEST UNIVERSITY OF TIMIWEST UNIVERSITY OF TIMIOARAOARAFACULTY OF CHEMISTRY, BIOLOGY, GEOGRAPHY

    DEPARTMENT OF BIOLOGYDEPARTMENT OF BIOLOGY--CHEMISTRYCHEMISTRY

    LAB. OF STRUCTURAL AND COMPUTAT IONAL PHYSICALLAB. OF STRUCTURAL AND COMPUTAT IONAL PHYSICAL--CHEMISTRY FORCHEMISTRY FORNANOSCIENCES & QSARNANOSCIENCES & QSAR(CFSCNQ)(CFSCNQ)

    Prof. dr. dr. habil. Mihai V. PUTZProf. dr. dr. habil. Mihai V. PUTZ

    Director CFSCNQDirector CFSCNQ

    [email protected][email protected]

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    Chemical Graph Theory is an important branch of

    Theoretical Chemistry.

    Its basic element is the so-called molecular

    graph G. Vertices V(G) of this graph denote

    molecular atoms and edges E(G) are the bonds of

    the molecule.

    Normally, G corresponds the carbon atomskeleton of the molecule. This is the hydrogen-

    depleted representation of the molecular

    graphs. Atomic valence is the vertex degree r.

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    Example Lets consider a connected graph G

    like this one with n nodes and m edges:

    n =10; m =11

    Chemically, G represents Naphtalene molecule

    with n carbon atoms and m bonds.

    Vertex degree r=2 or 3 corresponds to atomic

    valence. For carbon, silicon compounds r 4.

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    Graph Theory properties are transferred to

    molecular structures like the following TheFirst Theorem of Graph Theory:

    Any graph contains an even number ofvertices of odd degree r

    which becomes: Every molecule contains aneven number of atoms of odd valence

    Then C61 fullerene and others with odd

    carbon atoms are forbidden also by topology.

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    In Chemical Graph Theory gr aph invar i ant s or

    t opologi cal i ndices are used to correlate theproperties of molecules to their chemical

    structure.

    A t opologi cal i ndex is defined by a map from a

    graph G into a number or a finite string ofnumbers:

    Topologica l indicesshould be graph invar i ant,

    i.e. isomorphic graphs lead to the same

    topological index.

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    Isomor phic gr aphs

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    Isomor phic gr aphs

    EXERCISE are these graphs isomorphic ?

    See: Lecture Notes on GRAPH THEORY

    Tero Harju (2007), Department of Mathematics

    University of Turku, FIN-20014 Turku, Finland

    e-mail: [email protected]

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    Isomor phic gr aphs

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    An impor t ant t opological gr aph invar i ant t he Gr aph Ener gy

    See : Ivan Gutman, Bo Zhou and Boris Furtula

    The Laplacianenergy Like Invariant is an Energy Like Invariant

    MATCH Commun. Math. Comput. Chem. 64 (2010) 85-96

    ISSN 0340 - 6253 AND RELATED REFERENCES

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    Pr opert i es of t he Gr aph Ener gy

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    Then the total -electron energy of fullerenes and nanotubes

    is determined solely by their carbon atom content and depends

    very little on other structural features.

    Pr oper t i es of t he Gr aph Ener gy f or r egular gr aphs,

    i .e. whit vert ices wi t h t he same number of bonds (degr ee) r

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    Given two vertices u and v in V(G), we

    denote by d(u,v) or du,v the distancebetween u and v, i.e. the length of the

    shortest path connecting u and vby traveling

    along the graph edges (or molecular bonds).

    This distance belongs to the invariants of the

    graphs conveying crucial information about

    the structure.

    TECHNICALLY AND COMPUTATIONALLY THIS

    IS ONE OF SPECIALTIES OF Prof.PUTZs LAB

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    1 5 9 7 3

    2 6 10 8 4

    After an arbitrarilyarbitrarily numbering of the nodes

    we calculate the length dij of the shortestpath connecting pair wise the n atoms.

    n=10; m=11

    Some cases: d11=0 d12=d21=1

    d16=d19=2 .. Etc..

    dmax=d14=5

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    composing - with all dij entries - the Matrix

    D of the chemical distances of G:

    1 5 9 7 3

    2 6 10 8 4

    D 1 2 3 4 5 6 7 8 9 10

    1 0 1 4 5 1 2 3 4 2 3

    2 1 0 5 4 2 1 4 3 3 2

    3 4 5 0 1 3 4 1 2 2 3

    4 5 4 1 0 4 3 2 1 3 2

    5 1 2 3 4 0 3 2 3 1 2

    6 2 1 4 3 3 0 3 2 2 1

    7 3 4 1 2 2 3 0 3 1 28 4 3 2 1 3 2 3 0 2 1

    9 2 3 2 3 1 2 1 2 0 1

    10 3 2 3 2 2 1 2 1 1 0

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    D contains interesting structural information.

    Lets zoom in it first by sorting its rows:1 5 9 7 3

    2 6 10 8 4

    D wi

    1 0 1 1 2 2 3 3 4 4 5 13

    2 0 1 1 2 2 3 3 4 4 5 13

    3 0 1 1 2 2 3 3 4 4 5 134 0 1 1 2 2 3 3 4 4 5 13

    5 0 1 1 2 2 2 3 3 3 4 11

    6 0 1 1 2 2 2 3 3 3 4 11

    7 0 1 1 2 2 2 3 3 3 4 118 0 1 1 2 2 2 3 3 3 4 11

    9 0 1 1 1 2 2 2 2 3 3 8,5

    10 0 1 1 1 2 2 2 2 3 3 8,5

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    the action of D in possibly grouping

    structurally-equivalent atoms emerges:

    1 5 9 7 3

    2 6 10 8 4

    D wi

    1 0 1 1 2 2 3 3 4 4 5 13

    2 0 1 1 2 2 3 3 4 4 5 13

    3 0 1 1 2 2 3 3 4 4 5 134 0 1 1 2 2 3 3 4 4 5 13

    5 0 1 1 2 2 2 3 3 3 4 11

    6 0 1 1 2 2 2 3 3 3 4 11

    7 0 1 1 2 2 2 3 3 3 4 118 0 1 1 2 2 2 3 3 3 4 11

    9 0 1 1 1 2 2 2 2 3 3 8,5

    10 0 1 1 1 2 2 2 2 3 3 8,5

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    Row half-sum wi invariant provides atom-i

    contribution to Wiener index Wof G:

    W = ij dijW = wiw1 = 13, w5 = 11

    W = 109 w9= 8,5We call wi the Wiener weight of atom-i; lets

    zoom again in D by sorting by wi ..

    1 5 9 7 3

    2 6 10 8 4

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    the action of wi in suggesting possible

    most-stable atoms emerges:

    1 5 9 7 3

    2 6 10 8 4

    D wi

    9 0 1 1 1 2 2 2 2 3 3 8,5

    10 0 1 1 1 2 2 2 2 3 3 8,5

    5 0 1 1 2 2 2 3 3 3 4 11

    6 0 1 1 2 2 2 3 3 3 4 11

    7 0 1 1 2 2 2 3 3 3 4 11

    8 0 1 1 2 2 2 3 3 3 4 11

    1 0 1 1 2 2 3 3 4 4 5 13

    2 0 1 1 2 2 3 3 4 4 5 13

    3 0 1 1 2 2 3 3 4 4 5 13

    4 0 1 1 2 2 3 3 4 4 5 13

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    Exercise (HOMEWORK): for any (or all) of the

    below PAH structures:

    Write the ADJACENCY MATRIX

    Write the DISTANCE (BONDING) MATRIX

    Calculate the Wiener indexby making use of molecular symmetry

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    Much attention is devoted on FULLERENES.

    Luckily they admit a representation withplanar molecular graphs the Schlegel

    d iagramBuckminsterfullerene C60

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    Planar connected graphs fulfil Eulers theorem

    C20nv nf ne 2

    nv=20;ne=20*3/2=30

    nf=12whereisthe12th

    face?20+1230=2W=500=20*w1

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    Wiener index comutation of C20 fullerene

    C20 W=500=20*w1w1=25

    Shells Atoms k s*k1 3 3

    2 6 12

    3 6 18

    4 3 12

    5 1 550

    wi 25W=n*wi 500

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    Ri-prediction of

    the magic LEM:

    C28H4

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    Topological prediction of saturn like-fullerane C50H10 from C50D5h 10 equatorial reactive nodes (maximal wi ):

    NOT BAD AT ALL FOR A PURE TOPOLOGICAL WIENER BASEDNOT BAD AT ALL FOR A PURE TOPOLOGICAL WIENER BASED

    CALCULATIONS OF A MILLISECOND!CALCULATIONS OF A MILLISECOND!

    Ri-prediction of

    the SATURN:

    C50H10

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    Lets focus on the minimal vertices in green givingthe minimal contribution w to wiener index W

    w=8.5

    Minimal vertices are distinguished atoms in a graph,they are in fact the most compactly embedded in the

    structure.

    Now a question naturally arises: how to measurethe ability of the remaining atoms in contributing tothe overall compactness of graph G?

    1 5 9 7 3

    2 6 10 8 4

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    A possible solution consists in computing thefollowing invariant :

    = W/Nw 1

    = 1.282

    Index , called topological efficiency indextopological efficiency index, firstappeared in Ori Ottorino, Cataldo Franco and GraovacAnte (2009) Topological Ranking of C28 FullerenesReactivity, Fullerenes, Nanotubes and CarbonNanostructures, 17:3,308 323.

    1 5 9 7 3

    2 6 10 8 4

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    It is very interesting noticing that for the the

    buckminsterfullerene C60 Ih we have:

    = 1 C60 is in fact a very round hollow cage showing,

    for any of the N=60 nodes, the same {bim}={3 6 8

    10 10 10 8 3 1} coordination shells with M=9;wi=139=w and therefore W=N*w=8340. In this

    stable structure any node works as minimalminimal

    nodenode.

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    Assuming as a measure of sphericity it gives

    interesting (and sometime unexpected) results: Benzene is spherical =1;

    Closed square lattice (torus) is spherical

    Closed graphene lattice is spherical

    Sodalite closed zeolitic lattice

    is spherical =1 too and so onand so on..

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    Assuming to determine sphericity produces

    interesting (and sometime unexpected) results:

    C60 is spherical =1 as we said;

    C20

    polyhedron is also spherical =1

    Other fullerenes Cn have >1 so less

    spherical than C20but surely more stable

    Warning: better we try correlating and

    relative stability only among isomers of the

    same Cn fullerene.

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    is then the topological sphericityof a chemical graph

    The lower is the more spherical

    and stable the structure will be. So we adopted for invariant the

    new alias topological sphericitytopological sphericity

    indexindex

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    The minimum principle works BETTER on topological efficiency indextopological efficiency index

    1 as it has been successfully tested on C66 fullerene 4478 isomers, see

    Topological efficiency of C66 fullerene, D. Vukicevic, F. Cataldo , O. Ori,A. Graovac, Chemical Physics Letters 501 (2011) 442445.

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    Int. J. Mol. Sci. 2011, 12(11), 7934-7949;

    doi:10.3390/ijms12117934Topological Anisotropy of Stone-Wales Waves in Graphenic

    FragmentsOttorino Ori, Franco Cataldo and Mihai V. Putz

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    Index has been put in FULLERENE generator

    program by Prof. Peter Schwerdtfeger

    http://ctcp.massey.ac.nz/index.php?group=&page

    =fullerenes&menu=fullerenes

    free DOWNLAOD PLS USE IT

    Indices W andIndices W and tool quickly sieve interesting candidatestool quickly sieve interesting candidatesfor stable chemical structures (molecules, 1for stable chemical structures (molecules, 1--22--3D3D

    lattices, fractalslattices, fractals))

    WEST UNIVERSITY OF TIMIWEST UNIVERSITY OF TIMIOARAOARA

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    Questions ?

    Ottorino ORIActinium Chemical Research

    Rome

    [email protected]

    WEST UNIVERSITY OF TIMIWEST UNIVERSITY OF TIMIOARAOARAFACULTY OF CHEMISTRY, BIOLOGY, GEOGRAPHY

    DEPARTMENT OF BIOLOGYDEPARTMENT OF BIOLOGY--CHEMISTRYCHEMISTRYLAB. OF STRUCTURAL AND COMPUTAT IONAL PHYSICALLAB. OF STRUCTURAL AND COMPUTAT IONAL PHYSICAL--CHEMISTRY FORCHEMISTRY FOR

    NANOSCIENCES & QSARNANOSCIENCES & QSAR(CFSCNQ)(CFSCNQ)

    Prof. dr. dr. habil. Mihai V. PUTZProf. dr. dr. habil. Mihai V. PUTZ

    Director CFSCNQDirector CFSCNQ

    [email protected][email protected]